According to the results of the temperature dependencies of the intensity, linewidth and resonance field, we conclude that the peak at T(subscript M2) is a transition of antiferromagnetism.
通过对振线的强度、线宽和振场与温度依赖关系的讨论,我们得出T(下标M2)附近的峰对应着体系的反转变。
According to the results of the temperature dependencies of the intensity, linewidth and resonance field, we conclude that the peak at T(subscript M2) is a transition of antiferromagnetism.
通过对振线的强度、线宽和振场与温度依赖关系的讨论,我们得出T(下标M2)附近的峰对应着体系的反转变。
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